ライフサイエンスコーパス: GPa

1 from the starting 2.61 eV to 2.19 eV at 25.0 GPa accompanied by a color change from light yellow to d

2 ssy carbon at ultrahigh pressures up to 49.0 GPa by utilizing our recently developed double-stage lar

3 maintains graphite-like structure up to 49.0 GPa.

4 p(2)-bonded honey-comb structure, up to 49.0 GPa.

5 n, J(c)(H = 0) increases from 3.9 x 10(5) (0 GPa) to 1.3 x 10(6) (1.02 GPa) A/cm(2) at 2 K as the pre

6 locity values for the Young's modulus of 6.0 GPa.

7 a phase transition from F-43m to Imma at 7.0 GPa and explained the carrier-type inversion at approxim

8 d metallization of GaSb at approximately 7.0 GPa, which corresponds to a structural phase transition

9 rom 3.9 x 10(5) (0 GPa) to 1.3 x 10(6) (1.02 GPa) A/cm(2) at 2 K as the pressure is increased from no

10 re is increased from normal pressure to 1.02 GPa.

11 the resultant UTS estimate is 0.66 +/- 0.08 GPa.

12 t p-xylene crystallizes at approximately 0.1 GPa.

13 hape of the MOF hydroxyl vibration below 0.1 GPa.

14 nd W that possess strengths in excess of 1.1 GPa in as-printed and post-processed forms and tensile d

15 bsorption spectroscopies, measured up to 2.1 GPa in a diamond anvil cell on single crystals, are in e

16 exchange angle theta is decreased below 22.1 GPa, thus enhancing the PL quantum yield leading to Sn (

17 talline Cu(2)OSeO(3) by pressures up to 42.1 GPa through a series of phase transitions from the cubic

18 maximal hardness and elastic modulus of 46.1 GPa and 425 GPa, respectively.

19 temperature (Tc ) of 3.7 K, peaking at 47.1 GPa.

20 annealed at 250 degrees C at approximately 1 GPa pressure using diamond anvil cells (DACs) with heati

21 by the coexistence of iron and wustite) at 1 GPa and 1,400 degrees C.

22 sodium-magnesium aluminosilicate glass at 1 GPa at Tg, followed by sub-Tg annealing in-situ at 1 GPa

23 g, followed by sub-Tg annealing in-situ at 1 GPa.

24 to unlubricated surfaces under a constant 1 GPa Hertzian pressure in an ambient environment.

25 imetres, a slip/length ratio that implies >1 GPa stress drops.

26 esistivity (~8 GPa) and DC magnetization (~1 GPa) measurements.

27 composites with high mechanical modulus (~ 1 GPa) yet with liquid-like ion motions inside, and provid

28 al with a record high tensile strength of ~1 GPa and toughness of 9.74 MJ m(-3) .

29 p substances in high pressurized (of order 1 GPa) on nanobubbles.

30 temperature (T(g) ~ 483 degrees C) at P = 1 GPa pressure, in an argon atmosphere.

31 city-dependent UTSs increasing from 0.2 to 1 GPa in the available speed range, and 1.5 GPa extrapolat

32 can feature van-der-Waals pressures up to 1 GPa, producing a miniaturized high-pressure container fo

33 (3) GPa when K(T0)' = 6.6, or K(T0) = 166(1) GPa when K(T0)' is fixed at 4.

34 e and temperature range (pressure between 10 GPa and 110 GPa and temperature between 300 K and 4800 K

35 erconductor under high pressure exceeding 10 GPa.

36 es with remarkably high elastic modulus (>10 GPa) have been fabricated through the self-assembly of l

37 d, the c/a ratio reaches unity at ca. P = 10 GPa, where a monoclinic (M(c)) but metrically cubic tran

38 ural studies of feldspars are limited to ~10 GPa, and have shown that the dominant mechanism of press

39 commensurate structure (i-oF4) above 200(10) GPa, before finally adopting a monatomic form (oI2) abov

40 nto a metallic molecular form around 200(10) GPa.

41 ed-molecular structure (mC8, 130(10)-241(10) GPa) and the concomitant observation of a continuous ban

42 dopting a monatomic form (oI2) above 256(10) GPa.

43 etallic, ultraincompressible (K(0) = 428(10) GPa), and very hard (nanoindentation hardness 36.7(8) GP

44 lopes at different pressure intervals, 0 100 GPa, 100 250 GPa, 250-400 GPa, respectively, and the mom

45 ets emerge upon compression within the 0-100 GPa pressure range.

46 esis of cerium superhydride CeH(9) at 80-100 GPa in the laser-heated diamond anvil cell coupled with

47 maintained at low pressure, below about 100 GPa in Fe2MnAl and 50 GPa in Mn2FeAl.

48 cerium polyhydride CeH(9), formed above 100 GPa, presents a three-dimensional hydrogen network compo

49 ear spin states at pressures approaching 100 GPa (Meier, Annu.

50 imensional atomic hydrogen sublattice at 100 GPa.

51 iamond anvil cell at pressures exceeding 100 GPa is reported.

52 of pure iron carbonate at pressures over 100 GPa and temperatures over 2,500 K using single-crystal X

53 ff films, including CVD diamond films (~1000 GPa stiffness), as well as the transverse modulus of 2D

54 0.5 ns) after releasing of pressure from 11 GPa.

55 Our calculations up to 11 GPa and 1000 K indicate a higher concentration of bicarb

56 ature range (pressure between 10 GPa and 110 GPa and temperature between 300 K and 4800 K), only the

57 pe structure and is stable at pressures >113 GPa.

58 0 MPa, modulus varying over the range 14-116 GPa, and density varying over the range 880-14500 kg/m(3

59 hydrogen in its hexagonal phase I up to 123 GPa at room temperature.

60 ile strain (13.4%) and tensile strength (125 GPa).

61 The sharp shrinkage of the lattice at 13 GPa and the solid state of the decompressed sample we ob

62 s at very high pressures, e.g. FeH(5) at 130 GPa and LaH(10) at 170 GPa.

63 laser-generated shock compression (up to 130 GPa and 6,000 K along the MgSiO(3) glass Hugoniot).

64 ces its conductivity by about 2 folds at 132 GPa and 3000 K.

65 spin-paired and non-magnetic state at 60-133 GPa, while the presence of hydrogen has minimal effects

66 ven laser-heated diamond anvil cell from 135 GPa and 2,500 K to 154 GPa and 3,000 K.

67 This martensitic transformation begins at 14 GPa and is attributed to suppression of the local magnet

68 of the BC nanopapers stayed constant at ~ 14 GPa and ~ 120 MPa, respectively.

69 conditions of the basal magma ocean: 100-140 GPa, and 4000-6000 K.

70 The inherently strong CNCs (E(A) > 140 GPa) align into rigid, nematically ordered lamellae acro

71 Fe-Si and Fe-Si-O persisting to at least 140 GPa through a combination of laser-heated diamond-anvil

72 ities of solid Fe and Fe-Si alloys up to 144 GPa and 3300 K.

73 A modulus of 147 GPa for ThC at ambient pressure was obtained and the sto

74 th a similar structure at pressures above 15 GPa.

75 uO(6) polymorphs synthesized at 0, 6, and 15 GPa show B-site ordering, partial ordering, and disorder

76 ized by peak pressures possibly as low as 15 GPa for relatively long duration (on the order of 4 to 5

77 lagioclase is on average weakly shocked (<15 GPa) and examples of high shock states (>30 GPa; maskely

78 ers do not undergo phase transition up to 15 GPa, and in this pressure regime, their vibrational mode

79 results show that at low pressures up to 15 GPa, the carbon dioxide speciation is dominated by molec

80 Upon compression up to ~15 GPa, a new hexagonal phase of 2H-MoN(2) occurs, which is

81 kypaper/Parmax composite to 1145 MPa and 150 GPa, respectively, far exceeding those of Parmax and ali

82 rm that the sharp decrease in T(c) below 150 GPa is accompanied by continuous rhombohedral structural

83 arbon-hydrogen mixture at a pressure of ~150 GPa and a temperature of ~5000 K.

84 um remains stable in the hcp phase up to 150 GPa and 960 K.

85 orms at ~40 GPa and remains stable up to 150 GPa at least.

86 er-ablation pressure compresses Pb up to 150 GPa while keeping it solid, over two times as high in pr

87 rature has also been characterized up to 150 GPa.

88 d anvil cell from 135 GPa and 2,500 K to 154 GPa and 3,000 K.

89 K), reaching a maximum T(c) of 166 K at 157 GPa.

90 statically in diamond anvil cells (up to 157 GPa at room temperature) or dynamically by laser-generat

91 h combination of applied pressures up to 160 GPa and fields up to 65 T.

92 g phases in NaMgF(3) with compression to 162 GPa: NaMgF(3) (perovskite) -> NaMgF(3) (post-perovskite)

93 e pseudogap increases as dlnDelta*/dP = 0.17 GPa(-1).

94 dden in the cubic phase) remain until ca. 17 GPa, where a monoclinic-cubic transition is known in lea

95 sized with La atoms in an fcc lattice at 170 GPa upon heating to about 1000 K.

96 s, e.g. FeH(5) at 130 GPa and LaH(10) at 170 GPa.

97 continuously increases from 6 to 6.8 at 172 GPa.

98 igated the structure of SiO2 glass up to 172 GPa using high-energy X-ray diffraction.

99 and then a smaller linear decrease up to 172 GPa.

100 d-d breakdown) at pressures greater than 180 GPa.

101 III of solid hydrogen at pressures up to 183 GPa.

102 attice film has demonstrated modulus of 1.19 GPa and specific energy dissipation of 325.5 kJ/kg, surp

103 ave an elastic modulus of approximately 6-19 GPa, and hardness of approximately 120-170 MPa.

104 to the MIL-101 pores at a pressure below 0.2 GPa.

105 nd Raman spectra at low pressures (P = 1 - 2 GPa); and second, the c/a ratio reaches unity at ca. P =

106 y and compositional relationships in the 1.2 GPa Malaspina Pluton meant it was never likely to have d

107 compressive contact stresses as large as 1.2 GPa.

108 on x-ray diffraction experiments up to 105.2 GPa at room temperature using diamond anvil cells.

109 th a transition region between 14.1 and 25.2 GPa is observed, accompanying with a volume collapse ref

110 he tetragonal structure was complete by 29.2 GPa, ~5 GPa higher than the transition pressure obtained

111 elocity minima at 1.8 GPa for P wave and 3.2 GPa for S wave.

112 ificantly upon further compression up to 8.2 GPa.

113 at 96 hours (75.34 +/- 13.2 vs 134.4 +/- 8.2 GPa; p < 0.001).

114 duced visible photoluminescence (PL) above 2 GPa near 2 eV is observed.

115 Above 2 GPa, the energy absorption typically reaches 3-4 kJ/g; f

116 stable structure of methane hydrate above 2 GPa, where CH(4) molecules are located within H(2)O or D

117 pressure-induced superconductivity around 2 GPa.

118 We find moduli as low as 2 GPa, a value typical of soft materials and over one orde

119 rivial to a topological insulator phase at 2 GPa, which is caused by an energy gap close then reopen

120 At compressive stress below 2 GPa, relatively small amounts of energy (<0.3 kJ/g) are

121 ere determined at upper mantle conditions (2 GPa and 750-900 degrees C).

122 ical properties (Young's modulus exceeding 2 GPa).

123 ssurizing pure water to pressures of order 2 GPa or more.

124 high ultimate compressive strengths (over 2 GPa), high compressive failure strain (over 20%), and su

125 ), previously stabilized at high pressure (2 GPa) and high temperature (1600 K), is promising due to

126 emains nearly constant with pressure up to 2 GPa in good agreement with full-fledged density function

127 tetragonal phase is calculated to be 209(2) GPa and V(0) = 270(2) angstrom(3) when K(T0)' is fixed a

128 ined entrapment conditions, P(trap) = 6.5(2) GPa and T(trap) = 1125(32)-1140(33) degrees C, for the m

129 ases as dlnrho(100 K)/dP = -(10.5 +/- 0.2) %.GPa(-1).

130 Under the conditions of 15-20 GPa and 1800-2000 degrees C, spinel-type gamma-Si(3)N(4)

131 atography-mass spectrum, we found that at 20 GPa CHCF forms tilted columns with benzene and hexafluor

132 reduction along the stacking direction at 20 GPa in NOFN (18.8%) and 25 GPa in AOFN (8.7%) indicates

133 e increase in Si coordination observed at 20 GPa, we find no evidence for major structural changes oc

134 laments) with stiffness up to and beyond ~20 GPa, approaching the Young's moduli of many metal alloys

135 osed their formation at static pressures >20 GPa in a large planetary body, like diamonds formed deep

136 stal forms at 35 GPa and persists down to 20 GPa on decompression.

137 ered cubic (fcc) structure, stable above 200 GPa, and LaH8 a C2/m space group structure.

138 0%, and Young's modulus of approximately 200 GPa, offering one of the highest specific Young's modulu

139 With stability below 200 GPa, the superhydride is thus the closest analogue to so

140 At pressures up to 200 GPa, comparable to those present inside icy giant planet

141 tic (AFM) insulator at [Formula: see text]21 GPa whose AFM spin configuration is different from the A

142 Tc calculated for LaH10 is 274-286 K at 210 GPa.

143 tz transition between two Cmca phases at 220 GPa.

144 overed from hydrothermal synthesis above ~24 GPa where the [Formula: see text]-type (Ct) structure ap

145 as a function of pressure from ambient to 24 GPa using Monte-Carlo simulations constrained by high en

146 g direction at 20 GPa in NOFN (18.8%) and 25 GPa in AOFN (8.7%) indicates the pressure-induced breakd

147 erent pressure intervals, 0 100 GPa, 100 250 GPa, 250-400 GPa, respectively, and the moment collapses

148 room temperature, reaching 305-326 K at 250 GPa.

149 ure experiments of compounds stable to 24-26 GPa with Fe(4)O(5), Fe(5)O(6), Fe(7)O(9), and Fe(9)O(11)

150 rom 9.6 K at ambient to a peak at 23 K at 26 GPa and then drops as expected from the universal T(c)-P

151 ma phase has a large Young's modulus (ca. 26 GPa), a force of 0.1 muN can be generated under one lase

152 e-crystal X-ray diffraction studies up to 27 GPa, we report the discovery of new high-pressure polymo

153 Further, hardness of 8.28 GPa combined with modulus of 221.8 GPa was obtained in F

154 le tensile tests yield maximum values of 290 GPa for the Young's modulus and 5.8 GPa for the fracture

155 At 0.1-0.3 GPa expanded HDA (eHDA) and VHDA reach the same state be

156 etermined pressure difference of 0.8 +/- 0.3 GPa is due to deviation from lithostatic pressure.

157 Thus, 0.3 GPa sets the high-pressure limit for the possibility to

158 At P > 0.3 GPa the annealed amorphous ices no longer reach the same

159 ts at 24 hours (1.37 +/- 0.2 vs 6.13 +/- 0.3 GPa; p = 0.001) and 96 hours (5.57 +/- 0.5 vs 6.13 +/- 0

160 ) and 96 hours (5.57 +/- 0.5 vs 6.13 +/- 0.3 GPa; p = 0.006).

161 Here, we present experimental data at 1-3 GPa, 800 degrees C, and FMQ approximately -0.5 for the v

162 the acoustic velocities, measured up to 12.3 GPa using ultrasonic interferometry, exhibit velocity mi

163 h the tetragonal phase between 14.7 and 24.3 GPa.

164 ness values of 41.6 +/- 2.6 and 37.5 +/- 4.3 GPa, respectively.

165 superconductivity in In2 Se3 occurs at 41.3 GPa with a critical temperature (Tc ) of 3.7 K, peaking

166 tration of 3.6 vol.% approach 119.1 MPa, 5.3 GPa and 2.4 x 10(-4) S m(-1), with increases of 17%, 32.

167 into a high-density amorphous phase at ~6.3 GPa.

168 , thermodynamically metastable below about 3 GPa, shows a calculated negative P-T slope for its forma

169 However, its phase relations above 3 GPa and 1000 K are controversial.

170 t-pressed antigorite at pressures of 4 and 3 GPa, respectively, and at temperatures reaching 1073 K.

171 m, feldspars are stable at pressures up to 3 GPa and may persist metastably at higher pressures under

172 ulus of Mg(2)TiO(4) spinel is K(T0) = 148(3) GPa when K(T0)' = 6.6, or K(T0) = 166(1) GPa when K(T0)'

173 ctafluoronaphthalene (AOFN), up to 25 and 30 GPa, respectively, using single-crystal synchrotron X-ra

174 GPa) and examples of high shock states (>30 GPa; maskelynite) are uncommon.

175 affected by moderate to weak shock ( 5 to 30 GPa) we couple REE+Y abundances with FTIR analyses for F

176 appreciable local magnetic moments until 30 GPa to 40 GPa in the high-pressure phase of iron; howeve

177 the crystallization of chlorine at 1.15(30) GPa into an ordered orthorhombic structure (oC8), the ex

178 tronegativity in the pressure range of 0-300 GPa.

179 tions on the Hugoniot to pressures above 300 GPa.

180 g, which exhibit higher Young's moduli (1.33 GPa) than many synthetic polymers and biological filamen

181 de, NH(4)N(3), in a large-volume press at 33 GPa.

182 demonstrates outstanding hardness (up to 33 GPa) and fracture toughness (up to 5.2 MPa.m(1/2)), sign

183 on data show that CaO(3) crystal forms at 35 GPa and persists down to 20 GPa on decompression.

184 ter passing a broad valley between 20 and 36 GPa and reaches 90 K without any sign of saturation at 5

185 in film synthesis of high-hardness (up to 37 GPa) B(50)C(2) via chemical vapor deposition was achieve

186 n of the empty structure occurs at about 0.4 GPa.

187 tural silks, including a modulus of 11 +/- 4 GPa, even higher than natural spider silk.

188 the second neighbor C-C distance above 31.4 GPa.

189 highest values of the Vickers hardness (32.4 GPa), dynamic strength (1323 MPa), strain and toughness

190 ron x-ray total scattering method up to 38.4 GPa.

191 ectic curves were measured, beginning at 4.4 GPa and 165 degrees C (where it exists in a quadruple eq

192 4) qandilite was investigated to 50 and 40.4 GPa at room temperature using Raman spectroscopy and X-r

193 hat relatively mild pressure conditions (7.4 GPa at 300 K) are sufficient to transform ammonia monohy

194 orable compositions with a hardness above 40 GPa (at 0.5 N) are identified, proving this ensemble mod

195 However, at pressures above 40 GPa, T(c) rises rapidly without any sign of saturation u

196 e similar hardness values ( approximately 40 GPa at 0.49 N loading) as well as having a similar therm

197 work is isomorphic with ice Ih, forms at ~40 GPa and remains stable up to 150 GPa at least.

198 extending into the superhard region (HV > 40 GPa) have guided synthesis and identification of novel s

199 n is sluggish, occurring over a range of >40 GPa.

200 known materials have a Vickers hardness >=40 GPa at 0.5 N (applied force) and only 10 exceed this mar

201 )CO(3)-MgCO(3)) to pressures in excess of 40 GPa, far higher than any previous in situ study.

202 le local magnetic moments until 30 GPa to 40 GPa in the high-pressure phase of iron; however, no magn

203 e intervals, 0 100 GPa, 100 250 GPa, 250-400 GPa, respectively, and the moment collapses finally at 4

204 ness and elastic modulus of 46.1 GPa and 425 GPa, respectively.

205 ely, and the moment collapses finally at 450 GPa.

206 1 GPa in the available speed range, and 1.5 GPa extrapolated to the speeds expected in the sonicatio

207 uctural transition at [Formula: see text]1.5 GPa, and the other is from a ferromagnetic (FM) metal to

208 When the pressure is released to 1.5 GPa, emission can be triggered by above-band gap laser i

209 tion through a pressure cycle of 0 <--> 17.5 GPa.

210 rich fluids at 600-700 degrees C and 1.5-2.5 GPa and the discovery of methane-rich fluid inclusions i

211 ce of pressure-induced emission (PIE) at 2.5 GPa with a broad emission band and large Stokes shift fr

212 at lower shock pressures ( approximately 2.5 GPa), and amorphization and structural collapse at highe

213 N m(-1) and Young's modulus of 17.8 +/- 2.5 GPa, higher than any previously reported nucleic acid de

214 nsition via layer sliding, beginning at 28.5 GPa and not being completed up to around 60 GPa.

215 sodium acetate at 300 degrees C and 2.4-3.5 GPa and that over a broader range of pressures and tempe

216 sion (p-type to n-type) at approximately 4.5 GPa before metallization.

217 carrier-type inversion at approximately 4.5 GPa.

218 ic crystal with unit cell parameters (at 6.5 GPa and 20 degrees C) of a = 5.88 A, b = 6.59 A, c = 6.9

219 orphization transition in CaCO(3) at 3.9-7.5 GPa and temperature above 1000 K.

220 gonal structure was complete by 29.2 GPa, ~5 GPa higher than the transition pressure obtained by Rama

221 Above 50 GPa, the estimated coordination number continuously incr

222 ssure, below about 100 GPa in Fe2MnAl and 50 GPa in Mn2FeAl.

223 r from fourfold to sixfold between 15 and 50 GPa, in agreement with previous investigations.

224 ition from a Mott insulator to a metal at 50 GPa.

225 er-halide perovskites can decrease by ca. 50 GPa upon replacement of Cl with Br.

226 ered Cu-Cl perovskites require pressures >50 GPa to show a conductivity of 10(-4) S cm(-1) , whereas

227 of a new high-pressure phase above 40 to 50 GPa, although recently conjectured, remain unsolved to d

228 The Fd[Formula: see text]m phase at 500 GPa forms buckled honeycomb layers that give rise to a D

229 hout any sign of saturation up to 30 K at 51 GPa.

230 bon with a tensile strength of 1.60 +/- 0.55 GPa, a compressive strength approaching the theoretical

231 unresolved X-ray diffraction patterns at 55 GPa.

232 es 90 K without any sign of saturation at 56 GPa.

233 and IR wavelengths at pressures above ca. 56 GPa, suggesting the imminent closure of its optical band

234 ghness (62 MJ m(-3) ) and high stiffness (57 GPa).

235 n of ThC from B1 to P4/nmm at pressure of 58 GPa at ambient temperature.

236 -1) at only 2.6 GPa, and 0.17 S cm(-1) at 59 GPa.

237 compression under a mild pressure within 1.6 GPa considerably suppresses the carrier trapping, leadin

238 t, an ultra-high tensile strength of 2.4-2.6 GPa, a significant elongation of 4-10% and a good fractu

239 ity as high as 2x10(-3) S cm(-1) at only 2.6 GPa, and 0.17 S cm(-1) at 59 GPa.

240 se on shock release in only 2.4 ns from 33.6 GPa.

241 gth of 342 MPa and a Young's modulus of 43.6 GPa, respectively.

242 ed CaCO(3) melting curve overturn at about 6 GPa.

243 tor and metallic states can be closed near 6 GPa.

244 btained bulk modulus for 3R-MoN(2) is 77 (6) GPa, comparable with that of typical transition-metal di

245 riven to shock states between 0.49 and 16.60 GPa.

246 The metallic character of (MA)PbI3 above 60 GPa was confirmed using both IR reflectivity and variabl

247 t])[Formula: see text] At pressures above 60 GPa, [Formula: see text]O further changes the structural

248 GPa and not being completed up to around 60 GPa.

249 le tensile tests yields maximum values of 62 GPa for the Young's modulus and 0.70 GPa for the fractur

250 study are measured to be 0.85 GPa and 34.65 GPa, respectively.

251 is 1.7 eV band gap decreases to 0.3 eV at 65 GPa.

252 transition to antiferroelectric phase at 1.7 GPa adiabatic compression and become completely depolari

253 the Zr(0.5)Y(0.5)B(12) phase is 47.6 +/- 1.7 GPa at 0.49 N load, which is ~17% higher than that of it

254 effect of hydrostatic pressure up to P = 1.7 GPa on the fluctuation conductivity sigma'(T) and pseudo

255 uperconducting in decompression down to 10.7 GPa.

256 h approaching the theoretical limit of ~13.7 GPa, a substantial elastic limit of 20-30% and a low den

257 tetragonal (I4(1)/amd, No.141) phase at 14.7 GPa.

258 nt pressure to the pressure as high as 261.7 GPa, a record-high pressure up to which a known supercon

259 through a broad pressure range of 28.2-61.7 GPa, where a mixed semiconducting and metallic feature i

260 strength (826 MPa) and Young's modulus (65.7 GPa) owing to the large length and the alignment of nano

261 h the amorphization onset shifted to about 7 GPa.

262 Above 7 GPa, concomitantly to the nucleation of the amorphous ph

263 s of 62 GPa for the Young's modulus and 0.70 GPa for the fracture strength, significantly higher than

264 of ortho-hydrogen at low pressures, above 70 GPa, we observe a crossover in the nuclear spin statisti

265 nsition is observed at high pressure near 70 GPa.

266 s to a specific compressive strength of 9.79 GPa cm(3) g(-1), a value that surpasses that of nearly a

267 rite and gabbro were emplaced at 1.2 and 1.8 GPa are parts of the Western Fiordland Orthogneiss (WFO)

268 The 1.8 GPa Breaksea Orthogneiss includes suitably dense minor c

269 terferometry, exhibit velocity minima at 1.8 GPa for P wave and 3.2 GPa for S wave.

270 ratio from 0.3 to 0.42 at a pressure of 1.8 GPa, revealing a number of emergent field-induced phases

271 s of 8.28 GPa combined with modulus of 221.8 GPa was obtained in Fe-Mn-Co-Cr-Si-Cu HEA by annealing t

272 s of 290 GPa for the Young's modulus and 5.8 GPa for the fracture strength.

273 d anvil cells with pressures up to 54.0-62.8 GPa.

274 a much larger ultimate flexural modulus (7.8 GPa) than pure polymer electrolytes (20 MPa).

275 Ca(5)(Si(2)O(7))(CO(3))(2) tilleyite above 8 GPa.

276 llapse at higher pressures ( approximately 8 GPa).

277 gh the temperature dependent resistivity (~8 GPa) and DC magnetization (~1 GPa) measurements.

278 high pressure and high temperature, up to 8 GPa and 600 degrees C.

279 ecture with no phase change apparent up to 8 GPa.

280 achieved by the application of pressure to 8 GPa.

281 se diameter is as small as 17 nm and whose 8 GPa yield strength exceeds that of bulk nickel by up to

282 very hard (nanoindentation hardness 36.7(8) GPa) rhenium nitride pernitride Re(2)(N(2))(N)(2).

283 Beginning at 80 GPa and coincident with a transition to the previously p

284 ss relations in the ultrahard range (HV > 80 GPa) by examining single-crystal boron-doped diamond (BD

285 The X-ray diffraction (XRD) pattern at 0.84 GPa suggests that the crystallized p-xylene had a monocl

286 igated in this study are measured to be 0.85 GPa and 34.65 GPa, respectively.

287 isobaric heating at pressure 0.1 <= P <= 1.9 GPa is compared for five variants of high- (HDA) and ver

288 local structure of liquid gallium up to 1.9 GPa.

289 tals became completely depolarized under 3.9 GPa compression.

290 iamond anvil cell at pressures from 40 to 90 GPa and is recoverable at ambient conditions.

291 tal transition at high pressures close to 96 GPa is thus truly remarkable.

292 the increase in T(c) with dT(c)/dP = +1.82 K.GPa(-1) while the resistance decreases as dlnrho(100 K)/

293 (c) (dT(c)/dP) becomes 0.91 K/GPa and 0.75 K/GPa from magnetization and resistivity measurements resp

294 dependence of T(c) (dT(c)/dP) becomes 0.91 K/GPa and 0.75 K/GPa from magnetization and resistivity me

295 ith a Ki value of 143 nM against human liver GPa.

296 Imaging at ~100 nm resolution located GPa at sarcoplasmic reticulum (SR) junctional cisternae,

297 nanoparticle arrays to pressures of tens of GPa, demonstrating pressure-driven assembly beyond the q

298 that phosphorylated glycogen phosphorylase (GPa), glycogen synthase (GSa) - respectively activated a

299 us by up to six orders of magnitude from the GPa to kPa level at a controlled temperature within 28-4

300 -plastic straining is reported that utilizes GPa-level laser shocking at a high strain rate (depsilon